9,9-二-(3-(9-苯咔唑基))-2,7-芘基芴的光电性质

芴类化合物作为有机电致发光材料近年来引起了人们的广泛关注, 其具有高亮度和高工作效率等性能. 本论文采用量子化学方法研究了一种新型的芴类发光材料, 9,9-二-(3-(9-苯咔唑基))-2,7-芘基芴的光电性质. 具体研究内容包括基态和激发态几何结构、前线分子轨道、能隙、电离能、电子亲和势、重组能以及吸收光谱和发射光谱等. 理论计算结果表明, 9,9-二-(3-(9-苯咔唑基))-2,7-芘基芴发射光谱为450.6 nm, 其在电致发光器件应用上是一种具有开发前景和实用价值的蓝光发光材料.     

6-甲基-4-羟基嘧啶单体及二聚体激发态质子转移异构化反应及光谱的理论研究

采用ab initio HF理论的组态相关CIS方法和连续溶剂模型PCM, 分别在6-311+G*和6-31G水平上研究了6-甲基-4-羟基嘧啶单体及二聚体激发态质子转移的异构化反应; 对其反应势能面的研究发现, 单体基态和激发态的异构化反应一起可以形成四能级的分子电子体系, 而二聚体的却不能, 由此解释了单体和二聚体的紫外吸收光谱和荧光发射光谱均对应于酮式构型的原因. 利用混合含时密度泛函TD/MPW1PW91理论方法在溶剂存在下计算了标题物质的紫外吸收光谱和荧光发射光谱.     

3-(3′-吡啶基)-6-芳基-1，2，4-三唑并[3，4-b]-1，3，4-噻二唑衍生物基态和激发态性质

用密度泛函B3LYP方法对3-(3'-吡啶基)-6-芳基-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑衍生物(芳基为苯基、3-吡啶基和苯乙烯基)进行基态几何构型全优化,计算分子的电离势I_p和电子亲和势E_A等相关能量,并用Zerner间略微分重叠(ZINDO)和含时密度泛函(TDDFT)方法计算吸收光谱,用单组态相互作用方法(CIS)优化三种化合物分子的S_1激发态结构,分析其能量与发射光谱的关系,计算溶剂中分子的吸收和发射光谱,并与实验结果对照.计算结果表明,从3-(3'-吡啶基)-6-苯基-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑分子(化合物A)到3-(3'-吡啶基)-6-(3'-吡啶基)-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑分子(化合物B)以及3-(3'-吡啶基)-6-对乙烯苯基-1,2,4-三唑并[3,4-b]- 1,3,4-噻二唑分子(化合物C)的电子亲和势依次增大,愈来愈容易接受电子,吸收光谱和发射光谱红移.     

三苯胺取代蒽衍生物的结构和光学性质

采用DFT/B3LYP,HF,CIS及TD-DFT方法在6-31G(d)水平上研究了4种三苯胺取代蒽衍生物的结构和光学性质.计算结果表明:苯基、萘基、蒽基和芘基在蒽环9位进行修饰对分子的电子结构和光学性质影响微小.激发态结构弛豫主要发生在蒽环的键长;HOMO能级值较高,-5.0～-5.2eV,分子易产生空穴;蒽环9位取代基共轭面增加时,吸收光谱和发射光谱发生轻微红移,且发射光谱位于蓝光区域,约440nm.这4种衍生物均具有潜能作为性能优良的空穴型材料或蓝色发光材料应用于有机发光二极管中.     

3-(3’-吡啶基)-6-芳基-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑衍生物基态和激发态性质

用密度泛函B3LYP方法对3-(3’-吡啶基)-6-芳基-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑衍生物(芳基为苯基、3-吡啶基和苯乙烯基)进行基态几何构型全优化, 计算分子的电离势IP和电子亲和势EA等相关能量, 并用Zerner间略微分重叠(ZINDO)和含时密度泛函(TDDFT)方法计算吸收光谱, 用单组态相互作用方法(CIS)优化三种化合物分子的S1激发态结构, 分析其能量与发射光谱的关系, 计算溶剂中分子的吸收和发射光谱, 并与实验结果对照. 计算结果表明, 从3-(3’-吡啶基)-6-苯基-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑分子(化合物A)到3-(3’-吡啶基)-6-(3’-吡啶基)-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑分子(化合物B)以及3-(3’-吡啶基)-6-对乙烯苯基-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑分子(化合物C)的电子亲和势依次增大, 愈来愈容易接受电子, 吸收光谱和发射光谱红移.     

7-甲氧基香豆素-3-甲酰二乙醇胺的电子结构和光谱性质的理论研究

采用密度泛函的B3LYP和单激发组态相互作用(CIS)方法分别对基态和第一、第二单重激发态(S1和S2)结构进行优化,均采用6-31G(d)基组.在优化的基态和第一单重激发态的结构基础上,用含时密度泛函理论(TD-DFT),成功模拟了7-甲氧基香豆素-3-甲酰二乙醇胺的吸收光谱和荧光发射光谱,并用极化连续模型考虑了溶剂的影响.利用前线轨道、电荷密度差(CDD)和态密度(DOS)图分析了电子跃迁的特性.计算结果与实验结果吻合得很好.该量子计算方法对此类化合物的定性和定量研究是有效的.     

7-氮杂吲哚衍生物分子基态和激发态性质的理论研究

用从头算HF和密度泛函B3LYP方法对7-氮杂吲哚衍生物1,3-二(N-7-氮杂吲哚基)苯、1,3,5 三(N-7-氮杂吲哚基)苯和4,4′-二(N-7-氮杂吲哚基)联苯进行全优化, 计算分子的电离势IP和电子亲和势EA等相关能量, 并用ZINDO和TDDFT方法计算吸收光谱, 用CIS优化三种化合物分子的S1激发态结构, 并分析其能量与发射光谱的关系, 计算溶剂中分子的吸收和发射光谱, 并与实验结果对照. 计算结果表明, 从7-氮杂吲哚到上述三种衍生物依次愈来愈容易接受空穴, 吸收和发射光谱红移.     

3-吡咯烷基苯并蒽酮的电子结构和光谱性质

苯并蒽酮衍生物在新型荧光材料、非线性光学材料和液晶显示材料等领域有较大的应用前景.本文采用量子化学方法优化了3-吡咯烷基苯并蒽酮的基态几何结构和第一单重激发态的几何结构,并与X射线晶体衍射实验值进行了对比.利用含时密度泛函理论(TD-DFT)的不同泛函,计算了3-吡咯烷基苯并蒽酮在气相和溶剂中的吸收和发射光谱,考察了它的电子结构和光谱特征,并分析了不同泛函、基组以及溶剂效应对吸收和发射光谱的影响.计算结果表明:3-吡咯烷基苯并蒽酮的最强吸收和发射光谱都是具有π→π*跃迁特征的电荷转移(CT)态;泛函B3LYP能较好地重现实验吸收能;而对于具有分子内电荷转移特征的激发态,泛函MPWK能较好地重现实验发射能.溶剂效应的计算表明,不同极性的溶剂对3-吡咯烷基苯并蒽酮的吸收光谱和发射光谱的影响较小.理论预测的光谱与实验结果一致.     

14族杂环戊二烯分子(硅、锗、锡)的电子结构与光谱性质

14族杂原子取代的杂环戊二烯分子具有独特的光谱性质, 成为发光材料的明星分子. 为了更深层次地理解硅、锗、锡杂环戊二烯分子的光谱性质, 本文从理论上计算了它们的电子结构及其吸收和发射光谱. 分别采用密度泛函理论(DFT)和含时密度泛函理论(TD-DFT), 优化了硅、锗、锡杂环戊二烯分子基态和第一激发态的平衡构型, 计算了电子结构和振动性质. 在此基础上, 运用振动关联函数公式计算了吸收光谱和发射光谱. 得到的吸收光谱和发射光谱, 特别是发射光谱的半峰宽与现有的实验值吻合很好. 通过分析结构和光谱性质的关系, 指出光谱的性质主要取决于苯环转动对应的低频振动模式和中心环C—C键的伸缩振动对应的高频振动模式.     

醌型D-π-A类化合物AMTOE在不同溶剂中吸收和发射光谱的蓝移现象

采用连续介质模型(PCM)以及明确/连续的混合溶剂模型,运用密度泛函理论(DFT)和含时密度泛函理论(TD-DFT)方法,研究了溶剂极性对D-π-A类两性离子化合物1-(4-aza-4-methylphenyl)-2-trans-(4-oxyphenyl)ethane(AMTOE)分子几何、电子结构以及光谱性质的影响.计算结果表明,随着溶剂极性和超分子簇大小的增加,AMTOE基态(S0)分子几何从醌式结构向芳式结构转化.从基态(S0)到激发态(S1),化合物AMTOE醌式结构增强.从弱极性的氯仿溶液到强极性的水溶液,AMTOE分子的吸收光谱和发射光谱均发生蓝移,并且吸收光谱的蓝移程度大于发射光谱的蓝移程度,与实验现象定性一致.吸收光谱和发射光谱发生蓝移的原因是随着溶剂极性增强,HOMO轨道能级与LUMO轨道能级之间的能隙增大.对于具有明显电荷转移的AMTOE分子的溶剂化显色效应,长程矫正的含时密度泛函TD-CAM-B3LYP方法比传统的含时密度泛函TD-B3LYP方法更为合理.另外,明确/连续的混合溶剂模型能更好的描述该类体系在强极性溶剂中的溶剂化显色效应.     

2-苯基吡啶铱(Ⅲ)配合物及其衍生物光谱性质的理论研究

采用密度泛函理论B3PW91和UB3PW91方法, 分别对4种Ir(Ⅲ)配合物(ppy)₂Ir(acac)(1, ppy=2-苯基吡啶, acac=乙酰丙酮)、(npy)₂Ir(acac)(2, npy=2-萘-1-基吡啶)、(pq)₂Ir(acac)(3, pq=2-苯基喹啉)和(bzq)₂Ir(acac)(4, bzq=苯并喹啉)进行了基态和激发态的几何优化, 在此基础上用TD-DFT方法计算了吸收和发射光谱. 结果表明, 随着ppy配体上并苯环位置的变化, 参与最大吸收和发射的分子轨道能隙降低程度不同, 从而使配合物2, 3, 4的最大吸收和发射光谱都比配合物1发生红移, 其中在吡啶环上增加苯环对吸收光谱的影响最大. 这4个分子最大吸收波长的顺序为1<2<4<3, 而最大发射波长顺序则是1<4<3<2. 由于配合物2的两个苯环上H的强排斥作用降低了其共轭程度, 使分子发生很大程度的扭曲, 导致其斯托克位移最大.     

取代基对3(5)-(9-蒽基)吡唑光学性质的影响

使用密度泛函理论(DFT)B3LYP/6-31G(d)方法优化得到了3(5)-(9-蒽基)吡唑及其衍生物的基态(S₀)分子结构, 使用单激发组态相互作用(CIS)/6-31G(d)方法优化得到这些分子的第一单重激发态(S₁)的几何结构, 并使用含时密度泛函理论(TD-DFT)B3LYP/6-311++G(d,p)方法计算了它们的吸收和发射光谱. 计算结果表明, 与3(5)-(9-蒽基)吡唑相比, 无论取代基是吸电子基团还是供电子基团, 衍生物的吸收和发射峰均发生红移, 并且当取代基―R=―BH₂, ―CCl₃, ―CHO, ―NH₂时衍生物有较长的吸收波长和发射波长.     

Synthesis and Photophysical Properties of 3,6-Diphenyl-9-hexyl-9H-carbazole Derivatives Bearing Electron Withdrawing Groups

3,6-Diphenyl-9-hexyl-9H-carbazole derivatives bearing electron withdrawing groups, such as the formyl or the nitro-group in 4-positions of the phenyl substituents, were prepared and characterized. Their photophysical properties were evaluated and compared with those of the unsubstituted counterpart 3,6-diphenyl-9-hexyl-9H-carbazole. The electron withdrawing groups bearing compounds exhibited considerable red shifts of the absorption and the emission maxima. While 3,6-di(4-nitrophenyl)-9-hexyl-9H-carbazole emitted in the orange region of the visible spectrum with its emission maximum peaking at 585 nm, 3,6-di(4-formylphenyl)-9-hexyl-9H-carbazole gave a pure blue emission with a luminescence quantum yield of 95% peaking at 450 nm. Observed features were explained using quantum mechanical calculations and organic light emitting diodes using the formylphenyl substituted compound as emissive layer were built demonstrating the practical applicability of this class of compounds.     

Incorporating two different chromophores onto a silicon atom: the crystal structure and photophysical properties of 9‐{4‐[(9,9‐dimethyl‐9H‐fluoren‐2‐yl)dimethylsilyl]phenyl}‐9H‐carbazole

The crystal structure of the title bifunctional silicon‐bridged compound, C₃₅H₃₁NSi, (I), has been determined. The compound crystallizes in the centrosymmetric space group P2₁/c. In the crystal structure, the pairs of aryl rings in the two different chromophores, i.e. 9‐phenyl‐9H‐carbazole and 9,9‐dimethyl‐9H‐fluorene, are positioned orthogonally. In the crystal packing, no classical hydrogen bonding is observed. UV–Vis absorption and fluorescence emission spectra show that the central Si atom successfully breaks the electronic conjugation between the two different chromophores, and this was further analysed by density functional theory (DFT) calculations.     

Synthesis and Photophysical Properties of 3,6-Diphenyl-9-hexyl-9<Emphasis Type="Italic">H</Emphasis>-carbazole Derivatives Bearing Electron Withdrawing Groups

Summary. 3,6-Diphenyl-9-hexyl-9H-carbazole derivatives bearing electron withdrawing groups, such as the formyl or the nitro-group in 4-positions of the phenyl substituents, were prepared and characterized. Their photophysical properties were evaluated and compared with those of the unsubstituted counterpart 3,6-diphenyl-9-hexyl-9H-carbazole. The electron withdrawing groups bearing compounds exhibited considerable red shifts of the absorption and the emission maxima. While 3,6-di(4-nitrophenyl)-9-hexyl-9H-carbazole emitted in the orange region of the visible spectrum with its emission maximum peaking at 585 nm, 3,6-di(4-formylphenyl)-9-hexyl-9H-carbazole gave a pure blue emission with a luminescence quantum yield of 95% peaking at 450 nm. Observed features were explained using quantum mechanical calculations and organic light emitting diodes using the formylphenyl substituted compound as emissive layer were built demonstrating the practical applicability of this class of compounds.     

一种基于2, 2'-二吡啶胺功能化的新型空间位阻型9, 9'-二芳基芴的设计、合成及其光电性质研究

用2-溴吡啶通过乌尔曼反应修饰9-(4-苯胺基)-9-苯基芴合成了一种具有大体积空间位阻的双极性分子(PFPhDPy),这种化合物因其大的空间位阻、芴优异的双极型传输特性、共轭阻断结构以及吸电子的吡啶官能团而有望获得良好的热稳定性、稳定的无定形态、高的三线态能级和良好的双极性特征.热重分析曲线表明其失重5%的分解温度为336℃.差示扫描量热曲线显示将该化合物加热到190℃既没有熔化现象也没有结晶现象,意味着该化合物具有高的形貌稳定性.通过密度泛函理论计算,该化合物的最高占有轨道(HOMO)和最低未占有轨道(LUMO)完全分离,说明该化合物具有双极性特征,通过磷光光谱得到三线态能级为3.0 eV.紫外光谱显示该化合物不依赖于溶剂效应的三个特征吸收峰分别为276、298和308 nm.荧光光谱在二氯甲烷、乙酸乙酯、乙醇和乙腈溶剂中随着溶剂的极性增加光谱发生蓝移,其最大发射峰从390 nm转变为363 nm.另外,该化合物的结构分别通过基质辅助激光解析电离飞行时间质谱(MALDI-TOF MS)、氢核磁共振(¹H NMR)和碳核磁共振(¹³C NMR)谱进行了结构表征.     

Lattice energetics and thermochemistry of phenyl acridine-9-carboxylates and 9-phenoxycarbonyl-10-methylacridinium trifluoromethanesulphonates

The melting points and melting enthalpies of nine phenyl acridine-9-carboxylates—nitro-, methoxy- or halogen-substituted in the phenyl fragment—and their 9-phenoxycarbonyl-10-methylacridinium trifluoromethanesulphonate derivatives were determined by DSC. The volatilisation temperatures and enthalpies of phenyl acridine-9-carboxylates were either measured by DSC or obtained by fitting TG curves to the Clausius–Clapeyron relationship. For the compounds whose crystal structures are known, crystal lattice energies and enthalpies were determined computationally as the sum of electrostatic, dispersive and repulsive interactions. By combining the enthalpies of formation of gaseous phenyl acridine-9-carboxylates or 9-phenoxycarbonyl-10-methylacridinium trifluoromethanesulphonate ions, obtained by the DFT method, and the corresponding enthalpies of sublimation and/or crystal lattice enthalpies, the enthalpies of formation of the compounds in the solid phase were predicted. In the case of the phenyl acridine-9-carboxylates, the computationally predicted crystal lattice enthalpies correspond reasonably well with the experimentally obtained enthalpies of sublimation. The crystal lattices of phenyl acridine-9-carboxylates are stabilised predominantly by dispersive interactions between molecules, whilst the crystal lattices of their quaternary salts are stabilised by electrostatic interactions between ions.     

9-donor-substituted acridizinium salts: versatile environment-sensitive fluorophores for the detection of biomacromolecules

The absorption and steady-state emission properties of a series of N-alkyl- and N-aryl-9-aminoacridizinium derivatives and two 9-sulfanyl-substituted acridizinium derivatives were investigated. The N-alkyl derivatives and the 9-methylsulfanylacridizinium have an intense intrinsic fluorescence (phi(f) = 0.2-0.6), whereas the N-aryl-substituted compounds are virtually nonfluorescent in liquid solutions (phi(f) < or = 0.01). The emission intensity of the latter compounds significantly increases with increasing viscosity of the medium. It is demonstrated that the excited-state deactivation of the N-aryl-9-aminoacridizinium derivatives is due to two nonradiative processes: (i) torsional relaxation by rotation about the N-aryl bond and (ii) an electron-transfer process from an electron-donor substituted phenyl ring to the photoexcited acridizinium chromophore. The binding of several representative acridizinium derivatives to double-stranded DNA was studied by the spectrophotometric titrations and linear dichroism spectroscopy. The results give evidence that the prevailing binding mode is intercalation with binding constants in the range (0.5-5.0) x 10(5) M(-1) (in base pairs). Notably, the binding of most of the N-aryl-9-aminoacridizinium derivatives leads to a fluorescence enhancement by a factor of up to 50 upon binding to the biomacromolecules. Moreover, the addition of selected proteins, namely albumins, to N-(halogenophenyl)-9-aminoacridizinium ions in the presence of an anionic surfactant (sodium dodecyl sulfate) results in a 20-fold fluorescence enhancement. In each case, the emission enhancement is supposed to result from the hindrance of the torsional relaxation in the corresponding binding site of the biomacromolecule, which in turn suppresses the excited-state deactivation pathway.     

Synthesis and photophysical processes of 9-bromo-10-naphthalen-2-yl-anthracene

A novel luminescent compound, 9-bromo-10-naphthalen-2-yl-anthracene (BNA) is synthesized by Suzuki Cross-coupling reaction of 9-bromo-anthracene and naphthalene-2-boronic acid. The structure is characterized by (1)H NMR, IR and UV-vis spectroscopy. The photophysical processes of 9-bromo-10-naphthalen-2-yl-anthracene have been carefully investigated by UV-vis absorption and fluorescence spectra. The results show that the compound emits blue and blue-violet light. The emission spectra exhibit obvious solvent effect. With the difference in polarity of solvents, The emission spectra is not only slightly blue shift with the increase of the solvent polarity but also change on the intensity of fluorescence at room temperature .The light emitting can be quenched by electron donor, N,N-dimethylaniline (DMA). On adding gradually DMA into the solution of BNA, the emission intensities of fluorescence are gradually decreased. The quenching effect follows the Stern-Volmer equation.